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Finite-temperature Field Theory - Theoretical Physics (TIFR)

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Basics of Statistical <strong>Physics</strong> and Thermodynamics<br />

Scalar fields at finite <strong>temperature</strong><br />

Interacting scalar fields<br />

Partition function for scalar field theory<br />

Non-interacting examples<br />

Massive scalar fields<br />

◮ Specialize now to V (ϕ) = 1 2 m2 ϕ 2<br />

◮<br />

One free bosonic dof<br />

◮ Following rules of Gaussian integration<br />

{<br />

}<br />

(<br />

) −1/2<br />

ln Z = ln N det (−∂τ 2 − ∂i 2 + m 2 )<br />

= − 1 2 Tr ln (−∂2 τ − ∂i 2 + m 2 ) + const.<br />

◮ How to take a trace of an operator containing derivatives?<br />

◮<br />

Go to momentum space!<br />

logo<br />

Aleksi Vuorinen, CERN<br />

<strong>Finite</strong>-<strong>temperature</strong> <strong>Field</strong> <strong>Theory</strong>

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